High power flux cancelling current steering single core inductor

ABSTRACT

The present invention relates high power AC steering flux cancelling inductors and processes of making and using same. When properly configured and wired such inductors, separate the AC component and DC component of a high power current thus allowing the smaller AC fraction of the overall current to be carried by much smaller cross-sectional litz wires. Such high power AC steering flux cancelling inductors are more efficient at avoiding core saturation compared to standard inductors, yet they are less expensive without the need for large cross-sectional litz AC carrying wires. In addition to the aforementioned benefits, such high power AC steering flux cancelling inductor permits the levels of AC and DC current to be efficiently monitored as such currents are separated.

CROSS-REFERENCE TO RELATED APPLICATION

The present application claims priority to U.S. Provisional Application Ser. No. 63/325,186 filed Mar. 30, 2022, and U.S. Provisional Application Ser. No. 63/246,933 filed Sep. 22, 2021, the contents of both such provisional applications hereby being incorporated by reference in their entry.

RIGHTS OF THE GOVERNMENT

The invention described herein may be manufactured and used by or for the Government of the United States for all governmental purposes without the payment of any royalty.

FIELD OF THE INVENTION

The present invention relates to high power flux cancelling current steering single core inductors and processes of making and using same.

BACKGROUND OF THE INVENTION

Inductors are one of the heaviest and largest volume components in high power DC-DC converter and DC-AC inverter power electronic applications. Comprised of a soft magnetic core material and multiple turns of copper current carrying windings, inductors have power handling limitations based on both winding and core material fundamental properties. Under high current and high voltage operation, an inductor's core is subjected to very high magnetic fields (H) and may eventually saturate due to the high current and high voltage conditions. Saturation conditions define an upper limit on the power level that can be processed by a converter or power supply. In order to mitigate saturation conditions during converter operation, magnetic core cross-sectional area is increased and/or an air gap is introduced in the core's magnetic flux pathway. In addition, under high frequency and high current operations, skin depth considerations necessitate costly litz windings be used that consist of multi-strand wire weaved into the required gauge for the targeted power level. In some cases, these braided wires utilize more than one thousand strands of extremely fine magnet wires for very high frequency applications. Due to core saturation and winding wire frequency limitations, traditional high power inductors are made of large cores and are wound with litz wire resulting in inductors that dominate the cost, volume, and weight of inverter, power supply, and converter components. The subject invention not only provides a solution to both the need for high cost litz magnet wires but also mitigates core saturation limits and the need for large volume inductor cores. Inductors fabricated using the invention design paradigm result in energy storage devices that can be much reduced in size and cost.

The conventional geometry inductors have long been used for high voltage high power DC-DC converter applications. For high power, high frequency applications, conventional inductors must use large cross-sectional litz wires that consists of very fine magnet wires to prevent the losses due to the skin depth effect, and the large cross sectional inductor cores to prevent core saturation. Applicants recognized that the AC component of the current drove the need to use such large cross-sectional litz wires. As a result of such recognition, Applicants discovered that by properly configuring and wiring an inductor, the AC component and DC component of a high power current could be separated and that the separated AC component was a smaller fraction of the overall current. As the AC component was a smaller separated component of the overall current, such AC component could be handled by much smaller cross-sectional litz wires. Furthermore, Applicants recognized that such benefits could be obtained with a single core if the core material was judicially selected. As a result, Applicants' high power flux cancelling current steering single core inductor avoids core saturation, is much less expensive, has a more compact core, and large cross-sectional litz wires are not required. In addition to the aforementioned benefits, Applicants' high power flux cancelling current steering single core inductor permits the levels of AC and DC current to be efficiently monitored as such currents are separated.

SUMMARY OF THE INVENTION

The present invention relates high power AC steering flux cancelling inductors and processes of making and using same. When properly configured and wired such inductors, separate the AC component and DC component of a high power current thus allowing the smaller AC fraction of the overall current to be carried by much smaller cross-sectional litz wires. Such high power AC steering flux cancelling inductors are more efficient at avoiding core saturation compared to standard inductors, yet they are less expensive without the need for large cross-sectional litz AC carrying wires. In addition to the aforementioned benefits, such high power AC steering flux cancelling inductor permits the levels of AC and DC current to be efficiently monitored as such currents are separated.

BRIEF DESCRIPTION OF THE DRAWINGS

The accompanying drawings, which are incorporated in and constitute a part of this specification, illustrate embodiments of the present invention and, together with a general description of the invention given above, and the detailed description of the embodiments given below, serve to explain the principles of the present invention.

FIG. 1 is an isometric view from one embodiment of a high power flux cancelling current steering single core inductor.

FIG. 2 is a side view from one embodiment of a high power flux cancelling current steering single core inductor.

FIG. 3 is a top view from one embodiment of a high power flux cancelling current steering single core inductor.

FIG. 4 is an isometric view from a second embodiment of a high power flux cancelling current steering single core inductor.

FIG. 5 is an isometric view from a third embodiment of a high power flux cancelling current steering single core inductor.

FIG. 6 is an isometric view from a fourth embodiment of a high power flux cancelling current steering single core inductor.

FIG. 7 illustrates the magnetic relationships of the four windings included in the high power flux cancelling current steering single core inductor.

FIG. 8 is an example two-phase buck converter circuit utilizing a high power flux cancelling current steering single core inductor.

FIG. 9 is an example two-phase boost converter circuit utilizing a high power flux cancelling current steering single core inductor.

FIG. 10 is an example of current sensing utilizing a high power flux cancelling current steering single core inductor in parallel configuration.

FIG. 11 is an example of current sensing utilizing a high power flux cancelling current steering single core inductor in series configuration.

FIG. 12 is an example of current sensing utilizing a high power flux cancelling current steering single core inductor in an independent configuration.

FIG. 13 are example current signals through a high power flux cancelling current steering single core inductor in an independent configuration when V₁≠V₂.

DETAILED DESCRIPTION OF THE INVENTION Definitions

Unless specifically stated otherwise, as used herein, the terms “a”, “an” and “the” mean “at least one”.

As used herein, the terms “include”, “includes” and “including” are meant to be non-limiting.

Unless otherwise noted, all component or composition levels are in reference to the active portion of that component or composition, and are exclusive of impurities, for example, residual solvents or by-products, which may be present in commercially available sources of such components or compositions.

All percentages and ratios are calculated by weight unless otherwise indicated. All percentages and ratios are calculated based on the total composition unless otherwise indicated.

As used in this specification, the words “about,” “approximately,” or the like, when accompanying a numerical value, are to be construed as indicating a deviation as would be appreciated by one of ordinary skill in the art to operate satisfactorily for an intended purpose.

As used in this specification, the words “and/or” means, when referring to embodiments (for example an embodiment having elements A and/or B) that the embodiment may have element A alone, element B alone, or elements A and B taken together.

It should be understood that every maximum numerical limitation given throughout this specification includes every lower numerical limitation, as if such lower numerical limitations were expressly written herein. Every minimum numerical limitation given throughout this specification will include every higher numerical limitation, as if such higher numerical limitations were expressly written herein. Every numerical range given throughout this specification will include every narrower numerical range that falls within such broader numerical range, as if such narrower numerical ranges were all expressly written herein.

FIG. 1 depicts an isometric view of a first embodiment of a high power flux cancelling current steering single core inductor comprising a first winding (1), a second winding (2), a third winding (3), a fourth winding (4), a core (5) and winding turn passage (6).

FIG. 2 depicts a side view of the high power flux cancelling current steering single core inductor according to FIG. 1 showing first winding (1), second winding (2), third winding (3), fourth winding (4), and a core (5).

FIG. 3 depicts a top view of the high power flux cancelling current steering single core inductor according to FIG. 1 showing first winding (1), second winding (2), third winding (3), fourth winding (4), a core (5), a summation of flux (7) induced from first winding (1) and second winding (2) and a summation of flux (8) induced from third winding (3) and second winding (4).

FIG. 4 depicts an isometric view of a second embodiment of a high power flux cancelling current steering single core inductor comprising a first winding (1), a second winding (2), a third winding (3), a fourth winding (4), a core (5) and winding turn passage (6).

FIG. 5 depicts an isometric view of third embodiment of a high power flux cancelling current steering single core inductor comprising a first winding (1), a second winding (2), a third winding (3), a fourth winding (4), a core (5) and winding turn passage (6).

FIG. 6 depicts an isometric view of a fourth embodiment of a high power flux cancelling current steering single core inductor comprising a first winding (1), a second winding (2), a third winding (3), a fourth winding (4), a core (5) and winding turn passage (6).

High Power Flux Cancelling Current Steering Single Core Inductors and Article Comprising Same

For purposes of this specification, headings are not considered paragraphs and thus this paragraph is paragraph thirty-two of the present specification. The individual number of each paragraph above and below this paragraph can be determined by reference to this paragraph's number. In this paragraph thirty-two, Applicants disclose an inductor comprising:

-   -   a) a core; and     -   b) a first winding, a second winding, a third winding and a         fourth winding, two of said four windings being bulk AC         conducting windings and the remaining two of said four windings         being bulk DC conducting windings, said first winding and         optionally said second winding passing through said winding         passages of said core and after passing through said passages,         said first winding being partially wound around said core and         when said second winding passes through said winding passages of         said core, said second winding being partially wound around said         core after passing through said passages of said core, said         third winding and optionally said fourth winding passing through         said winding passages of said core and after passing through         said passages, said third winding being partially wound around         said core, and when said fourth winding passes through said         winding passages of said core, said fourth winding being         partially wound around said core after passing through said         passages of said core, said second winding being wound partially         through said passages of said core, or being wound completely         around said core and said fourth winding being wound partially         through said passages of said core, or being wound completely         around said core;         -   when a current comprising a DC current and an AC current is             supplied to said inductor, said bulk DC conducting windings             conducting at least 51%, preferably at least 70%, more             preferably at least 90%, most preferably at least 95% of             said DC current or about from 51% to about 99% of said DC             current and said bulk AC conducting windings conducting at             least 51%, preferably at least 70%, more preferably at least             90%, most preferably at least 99% of said AC current or from             about 51% to about 99.99% of said AC current and any of said             current's DC current not conducted by said bulk DC             conducting windings, said bulk DC conducting windings             conducting any of said current's AC current not conducted by             said bulk AC conducting windings, said windings each             independently having a resistivity at 20° C. of from about             1.5×10⁻⁸ Ohm-m to about 1.1×10⁻⁶ Ohm-m, preferably said             windings each independently having a resistivity at 20° C.             of from about 1.5×10⁻⁸ Ohm-m to about 4.2×10⁻⁷ Ohm-m, more             preferably said windings each independently having a             resistivity at 20° C. of from about 1.5×10⁻⁸ Ohm-m to about             1.4×10⁻⁷ Ohm-m, most preferably said windings each             independently having a resistivity at 20° C. of from about             1.5×10⁻⁸ Ohm-m to about 3.0×10⁻⁸ Ohm-m, said windings being             wound around said core pieces such that the following             inductor conditions are met when L₁=L₃, L₂=L₄, M₁₂=M₃₄, and             M₁₄=M₂₃:

Equation for Said First Winding

$V_{1} = {{L_{1}\frac{{di}_{1}}{dt}} + {M_{12}\frac{di_{2}}{dt}} - {M_{13}\frac{{di}_{3}}{dt}} - {M_{14}\frac{di_{4}}{dt}}}$

Equation For Said Second Winding

$V_{1} = {{M_{12}\frac{di_{1}}{dt}} + {L_{2}\frac{di_{2}}{dt}} - {M_{23}\frac{di_{3}}{dt}} - {M_{24}\frac{di_{4}}{dt}}}$

Equation For Said Third Winding

$V_{2} = {{{- M_{13}}\frac{{di}_{1}}{dt}} - {M_{23}\frac{{di}_{2}}{dt}} + {L_{3}\frac{di_{3}}{dt}} + {M_{34}\frac{di_{4}}{dt}}}$

Equation For Said Fourth Winding

$V_{2} = {{{- M_{14}}\frac{{di}_{1}}{dt}} - {M_{24}\frac{di_{2}}{dt}} + {M_{34}\frac{{di}_{3}}{dt}} + {L_{4}\frac{di_{4}}{dt}}}$

wherein for said equations the variables are defined as follows:

-   -   V₁ is a voltage across said first Winding;     -   V₁ is a voltage across said second Winding;     -   V₂ is a voltage across said third Winding;     -   V₂ is a voltage across said fourth Winding;     -   i₁ is a current in said first Winding;     -   i₂ is a current in said second Winding;     -   i₃ is a current in said third Winding;     -   i₄ is a current in said fourth Winding;     -   L₁ is a self inductance of said first Winding;     -   L₂ is a self inductance of said second Winding;     -   L₃ is a self inductance of said third Winding;     -   L₄ is a self inductance of said fourth Winding;     -   M₁₂ is a mutual inductance between said first Winding and said         second Winding;     -   M₁₃ is a mutual inductance between said first Winding and said         third Winding;     -   M₁₄ is a mutual inductance between said first Winding and said         fourth Winding;     -   M₂₃ is a mutual inductance between said second Winding and said         third Winding;     -   M₂₄ is a mutual inductance between said second Winding and said         fourth Winding;     -   M₃₄ is a mutual inductance between said third Winding and said         fourth Winding;         and said self and mutual inductances for said inductor         satisfying one of the following set of ideal conditions:         Criteria 1 and Criteria 1a; Criteria 1 and Criteria 1b; Criteria         2 and Criteria 2a; or Criteria 2 and Criteria 2b; wherein said         Criteria 1, Criteria 1a, Criteria 1b, Criteria 2, Criteria 2a,         and Criteria 2b are as follows:

L ₁ −M ₁₂≠0, M ₁₃ −M ₁₄≠0, and  (Criteria 1)

$\frac{di_{1}}{dt} = {\frac{di_{3}}{dt} = 0}$

-   -   If V₁≠V₂, then

$\frac{di_{2}}{dt}{and}\frac{di_{4}}{dt}$

-   -    are different values and:

(M ₁₂ −L ₂)=(M ₁₄ −M ₂₄)=0  (Criteria 1a)

-   -   If V₁=V₂, then

$\frac{{di}_{2}}{dt} = \frac{{di}_{4}}{dt}$

-   -    and:

(M ₁₂ −L ₂)=(M ₁₄ −M ₂₄)  (Criteria 1b)

or

M ₁₂ −L ₂≠0, M ₁₄ −M ₂₄≠0, and  (Criteria 2)

$\frac{di_{2}}{dt} = {\frac{di_{4}}{dt} = 0}$

-   -   If V₁≠V₂, then

$\frac{di_{1}}{dt}{and}\frac{di_{3}}{dt}$

-   -    are different values and:

(L ₁ −M ₁₂)=(M ₁₃ −M ₁₄)=0  (Criteria 2a)

-   -   If V₁=V₂, then

$\frac{{di}_{2}}{dt} = \frac{{di}_{4}}{dt}$

-   -    and:

(L ₁ −M ₁₂)=(M ₁₃ −M ₁₄)  (Criteria 2b).

The skilled artisan will understand that Criteria 1, 1a, 1b, 2, 2a and 2b are ideal in that they provide an acceptable set of criteria without undue mathematical complexity.

Applicants disclose the inductor of paragraph thirty-two having DC magnetic fluxes induced by said four windings, said core having a first and a second DC magnetic flux having the same direction, said first DC magnetic flux induced by one of said four windings and said second DC magnetic flux being induced by a separate winding of said four windings; and a third and a fourth DC magnetic flux having the same direction, said third DC magnetic flux induced by one of said four windings other than the windings that induce said first and a second DC magnetic fluxes and said fourth DC magnetic flux being induced by a winding of said four windings other than the windings that induce said first, second and third DC magnetic fluxes, said direction of said third and fourth DC magnetic fluxes being opposite the direction said first and second DC magnetic fluxes.

Applicants disclose the inductor of paragraphs thirty-two through thirty-three wherein said core comprises a material selected from the group consisting of soft magnetic materials, air and mixtures thereof, preferably said core comprises a soft magnetic material that comprises a material selected from the group consisting of a ferrimagnetic material, a ferromagnetic material and mixtures thereof, more preferably said core comprises a material selected from the group consisting of powder metals, solid metals, amorphous metal ribbon, ceramics and mixtures thereof, most preferably said core comprises a material selected from the group consisting of ferrites, nanocrystalline materials and mixtures thereof.

Applicants disclose the inductor of paragraphs thirty-two through thirty-four wherein said first, second, third and fourth windings comprise an electrically conductive material, preferably said first, second, third and fourth windings comprise an electrically conductive material selected from the group consisting of metals, superconductors, semiconductors, graphite, conductive polymers and mixtures thereof, more preferably said first, second, third, and fourth windings comprise an electrically conductive material selected from the group consisting of transition metals, post-transition metals, carbon fiber and mixtures thereof, most preferably said first, second, third, and fourth windings comprise an electrically conductive material selected from the group consisting of copper, aluminum, gold, silver and mixtures thereof.

Applicants disclose the inductor of paragraphs thirty-two through thirty-five said inductor having a DC flux cancellation of from about 20% to about 95%, preferably said inductor has a DC flux cancellation of from about 40% to about 95%, more preferably said inductor has a DC flux cancellation of from about 50% to about 90%, most preferably said inductor has a DC flux cancellation of from about 75% to about 90%.

Applicants disclose the inductor of thirty-two through thirty-six said inductor having a ratio of AC to DC current in said two other windings of from about 1:1 to about 1000000:1, preferably said inductor has a ratio of AC to DC current in each of said AC said two other windings from about 2:1 to about 10000:1, more preferably said inductor has a ratio of AC to DC current in each of said two other windings from about 3:1 to about 1000:1, most preferably said inductor has a ratio of AC to DC current in each of said two other windings from about 4:1 to about 100:1.

An article comprising an inductor according to paragraphs thirty-two through thirty-seven said article being selected from the group consisting of electrical current measurement or power converter and/or inverters, preferably said article being an electrical generation subsystem, electrical conditioning subsystem and/or distribution subsystem, most preferably said article being a vehicle power conditioning subsystem, a hybrid and/or electric vehicle charging station, a motor drive, a renewable energy conditioning, laser and/or maser drive, a telecommunication transmission power conditioning system, or a wireless power transmission power conditioning system.

This configuration takes advantage of the basic flux cancelling property of a coupled inductor design, particularly for use in power electronic control, conditioning, and distribution equipment, such as DC-DC converter energy storage elements. Such use cases present both saturation (DC) and skin depth (AC) limitations as the electrical power through the inductors contain both DC and AC currents. The major benefit of the invention is the ability to tailor the inductor to specific operating conditions such that a majority of the AC current is conducted only through one winding while the other winding carries a negligible amount of the total AC current. As a result, only one of the windings needs to be made with costly litz wire. In addition, since the subject invention consists of two inductors in one package, internal flux core saturation issues can be mitigated

The soft magnetic core materials needed to make the disclosed high power flux cancelling current steering single core inductors can be obtained from Spang & Company, 110 Delta Drive, Pittsburgh, Pa. 15238, Adams Magnetic Products Company, 888 Larch Avenue, Elmhurst, Ill. 60126, Dexter Magnetic Technologies, 1050 Morse Avenue, Elk Grove Village, Ill. 60007, and Hitachi Metals, Ltd., Shinagawa Season Terrace, 2-70, Konan 1-chome, Minato-ku, Tokyo 108-8224, Japan. Winding materials needed to make the disclosed high power flux cancelling current steering single core inductors can be obtained from: New England Wire Technologies, 130 North Main Street, Lisbon, N.H. 03585, and MWS Wire Industries, 3000 Camino Del Sol Oxnard, Calif. 93030

Process of Making a High Power Flux Cancelling Current Steering Single Core Inductor

Applicant discloses a process of making a high power flux cancelling current steering single core inductor. Inductor cores are first established per application requirements to meet physical, thermal, and electromagnetic properties. One core (5) is utilized as illustrated in the example in FIGS. 1, 2, 3, 4, 5, and 6 . Each core piece contains passages for windings to pass through the core pieces as shown in the example FIGS. 1, 4, 5, and 6 . With respect to the inductor disclosed herein, the core size, core material selection are dependent on the operating voltage of the application and appreciated by one of ordinary skill in the art of inductor or transformer design. With respect to the inductor disclosed herein, the core size, core material selection, wire size, and core through passage hole size are dependent on the power level of the application and appreciated by one of ordinary skill in the art of inductor or transformer design.

As appreciated by a skilled artisan in inductor or transformer design, the inductance of a high power flux cancelling current steering single core Inductor may be modified by adjusting number of winding turns, core size, core material selection, and/or gap dimensions. Each variable may be adjusted to satisfy the equations disclosed in this specification's “High power flux cancelling current steering single core Inductors and Article Comprising Same” section. Therefore, the number of winding turns need not to be the same between the first Winding (1) and the second Winding (2). Likewise, the number of winding turns need not the same between the third Winding (3) and the fourth Winding (4). The number of winding turns need not to be the same between the first Winding (1) and the third Winding (3) so long as the respective associated self-inductances are equivalent such as to satisfy the equations disclosed herein. Likewise, number of winding turns need not to be the same between the second Winding (2) and the Winding (4) so long as the respective associated self-inductances are equivalent such as to satisfy the equations disclosed in this specification's “High power flux cancelling current steering single core Inductors and Article Comprising Same” section.

The high power flux cancelling current steering single core Inductor consists of four windings of which the first Winding (1) and second Winding (2) are electrically connected at the input and output terminals; i.e., Winding 1 and Winding 2 are electrically parallel windings. Likewise, the third Winding (3) and fourth Winding (4) are electrically connected at the input and output terminals; i.e., Winding 3 and Winding 4 are electrically parallel windings. The first Winding (1) is partially wound around the Core (5) utilizing the through core piece winding passages where the second Winding (2) is optionally wound around the totality of the Core (5) or through the core piece winding passages as shown in example FIGS. 1, 4, 5, and 6 . Third Winding (3) is partially wound around the Core (5) utilizing the through core piece winding passages where the fourth Winding (4) is optionally wound around the totality of the Core (5) or through the core winding passages as shown in example FIGS. 1, 4, 5, and 6 . The number of turns for the first Winding (1) and third Winding (3) are equivalent; likewise, the number of turns for the second Winding (2) and fourth Winding (4) are equivalent.

The first Winding (1) and second Winding (2) are wound in the same orientation in accordance with the equations disclosed in this specification's “High Power Flux Cancelling Current Steering Single Core Inductors and Article Comprising Same” section. Likewise, the third Winding (3) and fourth Winding (4) are wound in the same orientation in accordance with the equations disclosed in this specification's “High power flux cancelling current steering single core Inductors and Article Comprising Same” section. The winding orientations are such that the DC flux induced by each set of windings is in opposition; i.e., DC flux (7) induced by first Winding (1) and second Winding (2) opposes that of the DC flux (8) induced by third Winding (3) and fourth Winding (4).

The AC current through each winding can be controlled by one of the criteria listed paragraph thirty-one of this specification. Adjusting the core materials, core dimensions, gap distances, and number turns of the windings will tailor the self and mutual inductances to meet the desired set of criteria.

DC current through the first Winding (1) and second Winding (2) can be controlled by the ratio of the first Winding's DC resistance and the second Winding's DC resistance. Similarly, DC current through the third Winding (3) and fourth Winding (4) can be controlled by the ratio of the third Winding's DC resistance and fourth Winding's DC resistance. A significant advantage of the inductors that Applicants disclose and/or claim in this specification is that the windings that carry most of the AC current can be wound using litz type wire that consists of strands 12 American Wire Gauge (AWG) or greater gauge, and the windings that carry little AC current need not be made with expensive litz wire. Precise wire gauge selection is dependent on the application and appreciated by one of ordinary skill in the art of inductor or transformer design.

Applicants disclose a process, in this paragraph forty-seven, of making an inductor comprising winding, around a core, a first winding, a second winding, a third winding and a fourth winding, said step of winding said first winding, said second winding, said third winding and said fourth winding about said core comprising winding said first winding, said second winding, said third winding and said fourth winding around said core pieces such that the following inductor conditions are met when L₁=L₃, L₂=L₄, M₁₂=M₃₄, and M₁₄=M₂₃:

Equation For Said First Winding

$V_{1} = {{L_{1}\frac{{di}_{1}}{dt}} + {M_{12}\frac{di_{2}}{dt}} - {M_{13}\frac{{di}_{3}}{dt}} - {M_{14}\frac{di_{4}}{dt}}}$

Equation For Said Second Winding

$V_{1} = {{M_{12}\frac{di_{1}}{dt}} + {L_{2}\frac{di_{2}}{dt}} - {M_{23}\frac{{di}_{3}}{dt}} - {M_{24}\frac{di_{4}}{dt}}}$

Equation For Said Third Winding

$V_{2} = {{{- M_{13}}\frac{di_{1}}{dt}} - {M_{23}\frac{{di}_{2}}{dt}} + {L_{3}\frac{di_{3}}{dt}} + {M_{34}\frac{{di}_{4}}{dt}}}$

Equation For Said Fourth Winding

$V_{2} = {{{- M_{14}}\frac{{di}_{1}}{dt}} - {M_{24}\frac{{di}_{2}}{dt}} + {M_{34}\frac{{di}_{3}}{dt}} + {L_{4}\frac{di_{4}}{dt}}}$

-   -   wherein for said equations the variables are defined as follows:         -   V₁ is a voltage across said first Winding;         -   V₁ is a voltage across said second Winding;         -   V₂ is a voltage across said third Winding;         -   V₂ is a voltage across said fourth Winding;         -   i₁ is a current in said first Winding;         -   i₂ is a current in said second Winding;         -   i₃ is a current in said third Winding;         -   i₄ is a current in said fourth Winding;         -   L₁ is a self inductance of said first Winding;         -   L₂ is a self inductance of said second Winding;         -   L₃ is a self inductance of said third Winding;         -   L₄ is a self inductance of said fourth Winding;         -   M₁₂ is a mutual inductance between said first Winding and             said second Winding;         -   M₁₃ is a mutual inductance between said first Winding and             said third Winding;         -   M₁₄ is a mutual inductance between said first Winding and             said fourth Winding;         -   M₂₃ is a mutual inductance between said second Winding and             said third Winding;         -   M₂₄ is a mutual inductance between said second Winding and             said fourth Winding;         -   M₃₄ is a mutual inductance between said third Winding and             said fourth Winding;     -   and said self and mutual inductances for said inductor         satisfying one of the following set of ideal conditions:         Criteria 1 and Criteria 1a; Criteria 1 and Criteria 1b; Criteria         2 and Criteria 2a; or Criteria 2 and Criteria 2b; wherein said         Criteria 1, Criteria 1a, Criteria 1b, Criteria 2, Criteria 2a,         and Criteria 2b are as follows:

L ₁ −M ₁₂≠0, M ₁₃ −M ₁₄≠0, and  (Criteria 1)

$\frac{{di}_{1}}{dt} = {\frac{{di}_{3}}{dt} = 0}$

-   -   -   If V₁≠V₂, then

$\frac{di_{2}}{dt}{and}\frac{di_{4}}{dt}$

-   -   -    are different values and:

(M ₁₂ −L ₂)=(M ₁₄ −M ₂₄)=0  (Criteria 1a)

-   -   -   If V₁=V₂, then

$\frac{di_{2}}{dt} = \frac{di_{4}}{dt}$

-   -   -    and:

(M ₁₂ −L ₂)=(M ₁₄ −M ₂₄)  (Criteria 1b)

or

M ₁₂ −L ₂≠0, M ₁₄ −M ₂₄≠0, and  (Criteria 2)

$\frac{{di}_{2}}{dt} = {\frac{{di}_{4}}{dt} = 0}$

-   -   -   If V₁≠V₂, then

$\frac{di_{1}}{dt}{and}\frac{di_{3}}{dt}$

-   -   -    are different values and:

(L ₁ −M ₁₂)=(M ₁₃ −M ₁₄)=0  (Criteria 2a)

-   -   -   If V₁=V₂, then

$\frac{di_{2}}{dt} = \frac{di_{4}}{dt}$

-   -   -    and:

(L ₁ −M ₁₂)=(M ₁₃ −M ₁₄)  (Criteria 2b).

The skilled artisan will understand that Criteria 1, 1a, 1b, 2, 2a and 2b are ideal in that they provide an acceptable set of criteria without undue mathematical complexity.

Applicants disclose the process of paragraph forty-seven wherein said first winding, said second winding, said third winding and said fourth winding around said core such that said first winding and optionally said second winding pass through said winding passages of said core and after passing through said passages, said first winding is partially wound around said core and when said second winding passes through said winding passages of core, said second winding is partially wound around said core after passing through said passages of said core, said third winding and optionally said fourth winding passing through said winding passages of said core and after passing through said passages, said third winding is partially wound around said core, and when said fourth winding passes through said winding passages of said core, said fourth winding is partially wound around said core after passing through said passages of said core, said second winding is wound partially through said passages of said core, or being wound completely around said core and said fourth winding is wound partially through said passages of said core, or being wound completely around said core.

Applicants disclose a process according to paragraphs forty-seven through forty-eight wherein said inductor is the inductor of paragraphs thirty-two through thirty-seven.

Test Methods

Applicant discloses a test method of a high power flux cancelling current steering single core inductor. After a High power flux cancelling current steering single core Inductor is assembled using the previously described process, the self and mutual inductor parameters can be measured using a standard LCR meter to meet the desired criteria. Each self-inductance and mutual inductance property can be determined using a Keysight Technologies, E4980A Precision LCR Meter following the procedure outlined in the Keysight Technologies E4980A/AL Precision LCR Meter User's Guide, Inductance Measurements Section. In situ measurements using an oscilloscope from Teledyne LeCroy, to measure inductor currents and differentially measure inductor voltages, can verify that the equations used in Applicants claims and found in paragraph thirty-one of this specification are satisfied. Suppliers of such instruments are Keysight Technologies of 1900 Garden of the Gods Road, Colorado Springs, Colo. 80907-3423 and Teledyne LeCroy of 700 Chestnut Ridge Road, Chestnut Ridge, N.Y. 10977-6499.

Example

The following example embodiment illustrates the particular properties and advantages of the present invention. Furthermore, this is an example of reduction to practice of the present invention and confirmation that the principles described in the present invention are therefore valid but should not be construed as in any way limiting the scope of the invention.

Example 1 embodiment similar to that shown in FIG. 1 is simulated with the constraints described in the claims and:

L₁−M₁₂≠0, M₁₃−M₁₄≠0, and

$\frac{{di}_{1}}{dt} = {\frac{{di}_{3}}{dt} = 0}$

If V₁=V₂, then

$\frac{{di}_{2}}{dt}{and}\frac{di_{4}}{dt}$

are similar values and (M₁₂−L₂)=(M₁₄−M₂₄)

Specifically, said Example 1 is simulated with self and mutual inductances of:

-   -   L₁=L₃=86.7 μH     -   L₂=L₄=54.1 pH     -   M₁₂=40.5 μH     -   M₁₃=72.3 μH     -   M₁₄=37.2 pH     -   M₂₄=50.2 μH         From these values, simulation indicated the AC portions of         i_(1ac), and i_(3ac) is minimal.

The aforementioned example embodiment is simulated for a current sensing application. Such an embodiment is equally appropriate for converter and inverter functions which are suitable for electrical generation, conditioning, and distribution subsystems, within vehicle power conditioning subsystems, hybrid and/or electric vehicle charging stations, motor drives, renewable energy conditioning, laser/maser drives, telecommunication transmission power conditioning, or wireless power transmission power conditioning.

Every document cited herein, including any cross referenced or related patent or application and any patent application or patent to which this application claims priority or benefit thereof, is hereby incorporated herein by reference in its entirety unless expressly excluded or otherwise limited. The citation of any document is not an admission that it is prior art with respect to any invention disclosed or claimed herein or that it alone, or in any combination with any other reference or references, teaches, suggests or discloses any such invention. Further, to the extent that any meaning or definition of a term in this document conflicts with any meaning or definition of the same term in a document incorporated by reference, the meaning or definition assigned to that term in this document shall govern.

While the present invention has been illustrated by a description of one or more embodiments thereof and while these embodiments have been described in considerable detail, they are not intended to restrict or in any way limit the scope of the appended claims to such detail. Additional advantages and modifications will readily appear to those skilled in the art. The invention in its broader aspects is therefore not limited to the specific details, representative apparatus and method, and illustrative examples shown and described. Accordingly, departures may be made from such details without departing from the scope of the general inventive concept. 

What is claimed is:
 1. An inductor comprising: a) a core; and b) a first winding, a second winding, a third winding and a fourth winding, two of said four windings being bulk AC conducting windings and the remaining two of said four windings being bulk DC conducting windings, said first winding and optionally said second winding passing through said winding passages of said core and after passing through said passages, said first winding being partially wound around said core and when said second winding passes through said winding passages of said core, said second winding being partially wound around said core after passing through said passages of said core, said third winding and optionally said fourth winding passing through said winding passages of said core and after passing through said passages, said third winding being partially wound around said core, and when said fourth winding passes through said winding passages of said core, said fourth winding being partially wound around said core after passing through said passages of said core, said second winding being wound partially through said passages of said core, or being wound completely around said core and said fourth winding being wound partially through said passages of said core, or being wound completely around said core; when a current comprising a DC current and an AC current is supplied to said inductor, said bulk DC conducting windings conducting at least 51% of said DC current and said bulk AC conducting windings conducting at least 51% of said AC current and any of said current's DC current not conducted by said bulk DC conducting windings, said bulk DC conducting windings conducting any of said current's AC current not conducted by said bulk AC conducting windings, said windings each independently having a resistivity at 20° C. of from about 1.5×10⁻⁸ Ohm-m to about 1.1×10⁻⁶ Ohm-m, said windings being wound around said core pieces such that the following inductor conditions are met when L₁=L₃, L₂=L₄, M₁₂=M₃₄, and M₁₄=M₂₃: Equation For Said First Winding $V_{1} = {{L_{1}\frac{{di}_{1}}{dt}} + {M_{12}\frac{di_{2}}{dt}} - {M_{13}\frac{{di}_{3}}{dt}} - {M_{14}\frac{di_{4}}{dt}}}$ Equation For Said Second Winding $V_{1} = {{M_{12}\frac{di_{1}}{dt}} + {L_{2}\frac{di_{2}}{dt}} - {M_{23}\frac{{di}_{3}}{dt}} - {M_{24}\frac{di_{4}}{dt}}}$ Equation For Said Third Winding $V_{2} = {{{- M_{13}}\frac{{di}_{1}}{dt}} - {M_{23}\frac{{di}_{2}}{dt}} + {L_{3}\frac{di_{3}}{dt}} + {M_{34}\frac{di_{4}}{dt}}}$ Equation For Said Fourth Winding $V_{2} = {{{- M_{14}}\frac{{di}_{1}}{dt}} - {M_{24}\frac{{di}_{2}}{dt}} + {M_{34}\frac{{di}_{3}}{dt}} + {L_{4}\frac{di_{4}}{dt}}}$ wherein for said equations the variables are defined as follows: V₁ is a voltage across said first Winding; V₁ is a voltage across said second Winding; V₂ is a voltage across said third Winding; V₂ is a voltage across said fourth Winding; i₁ is a current in said first Winding; i₂ is a current in said second Winding; i₃ is a current in said third Winding; i₄ is a current in said fourth Winding; L₁ is a self inductance of said first Winding; L₂ is a self inductance of said second Winding; L₃ is a self inductance of said third Winding; L₄ is a self inductance of said fourth Winding; M₁₂ is a mutual inductance between said first Winding and said second Winding; M₁₃ is a mutual inductance between said first Winding and said third Winding; M₁₄ is a mutual inductance between said first Winding and said fourth Winding; M₂₃ is a mutual inductance between said second Winding and said third Winding; M₂₄ is a mutual inductance between said second Winding and said fourth Winding; M₃₄ is a mutual inductance between said third Winding and said fourth Winding; and said self and mutual inductances for said inductor satisfying one of the following set of conditions: Criteria 1 and Criteria 1a; Criteria 1 and Criteria 1b; Criteria 2 and Criteria 2a; or Criteria 2 and Criteria 2b; wherein said Criteria 1, Criteria 1a, Criteria 1b, Criteria 2, Criteria 2a, and Criteria 2b are as follows: L ₁ −M ₁₂≠0, M ₁₃ −M ₁₄≠0, and  (Criteria 1) $\frac{{di}_{1}}{dt} = {\frac{{di}_{3}}{dt} = 0}$ If V₁≠V₂, then $\frac{di_{2}}{dt}{and}\frac{di_{4}}{dt}$  are different values and: (M ₁₂ −L ₂)=(M ₁₄ −M ₂₄)=0  (Criteria 1a) If V₁=V₂, then ${\frac{di_{2}}{dt} = \frac{di_{4}}{dt}} = 0$  and: (M ₁₂ −L ₂)=(M ₁₄ −M ₂₄)  (Criteria 1b) or M ₁₂ −L ₂≠0, M ₁₄ −M ₂₄≠0, and  (Criteria 2) $\frac{{di}_{2}}{dt} = {\frac{{di}_{4}}{dt} = 0}$ If V₁≠V₂, then $\frac{di_{1}}{dt}{and}\frac{di_{3}}{dt}$  are different values and: (L ₁ −M ₁₂)=(M ₁₃ −M ₁₄)=0  (Criteria 2a) If V₁=V₂, then $\frac{di_{2}}{dt} = \frac{di_{4}}{dt}$  and: (L ₁ −M ₁₂)=(M ₁₃ −M ₁₄)  (Criteria 2b).
 2. The inductor of claim 1 wherein when a current comprising a DC current and an AC current is supplied to said inductor, said bulk DC conducting windings conducting at least 70% of said DC current and said bulk AC conducting windings conducting at least 70% of said AC current and any of said current's DC current not conducted by said bulk DC conducting windings, said bulk DC conducting windings conducting any of said current's AC current not conducted by said bulk AC conducting windings, said windings each independently having a resistivity at 20° C. of from about 1.5×10⁻⁸ Ohm-m to about 4.2×10⁻⁷ Ohm-m.
 3. The inductor of claim 2 wherein when a current comprising a DC current and an AC current is supplied to said inductor, said bulk DC conducting windings conducting at least 90% of said DC current and said bulk AC conducting windings conducting at least 90% of said AC current and any of said current's DC current not conducted by said bulk DC conducting windings, said bulk DC conducting windings conducting any of said current's AC current not conducted by said bulk AC conducting windings, said windings each independently having a resistivity at 20° C. of from about 1.5×10⁻⁸ Ohm-m to about 1.4×10⁻⁷ Ohm-m.
 4. The inductor of claim 3 wherein when a current comprising a DC current and an AC current is supplied to said inductor, said bulk DC conducting windings conducting at least 95% of said DC current and said bulk AC conducting windings conducting at least 99% of said AC current and any of said current's DC current not conducted by said bulk DC conducting windings, said bulk DC conducting windings conducting any of said current's AC current not conducted by said bulk AC conducting windings, said windings each independently having a resistivity at 20° C. of from about 1.5×10⁻⁸ Ohm-m to about 3.0×10⁻⁸ Ohm-m.
 5. The inductor of claim 1 having DC magnetic fluxes induced by said four windings said core having a first and a second DC magnetic flux having the same direction, said first DC magnetic flux induced by one of said four windings and said second DC magnetic flux being induced by a separate winding of said four windings; and a third and a fourth DC magnetic flux having the same direction, said third DC magnetic flux induced by one of said four windings other than the windings that induce said first and a second DC magnetic fluxes and said fourth DC magnetic flux being induced by a winding of said four windings other than the windings that induce said first, second and third DC magnetic fluxes, said direction of said third and fourth DC magnetic fluxes being opposite the direction said first and second DC magnetic fluxes.
 6. The inductor of claim 1 wherein said core comprising a material selected from the group consisting of soft magnetic materials, air and mixtures thereof.
 7. The inductor of claim 6 wherein said core comprises a soft magnetic material that comprises a material selected from the group consisting of a ferrimagnetic material, a ferromagnetic material and mixtures thereof
 8. The inductor of claim 7 wherein said core comprises a material selected from the group consisting of powder metals, solid metals, amorphous metal ribbon, ceramics and mixtures thereof
 9. The inductor of claim 8 wherein said core comprises a material selected from the group consisting of ferrites, nanocrystalline materials and mixtures thereof
 10. The inductor of claim 1 wherein said first, second, third and fourth windings comprise an electrically conductive material.
 11. The inductor of claim 10 wherein said first, second, third and fourth windings comprise an electrically conductive material selected from the group consisting of metals, superconductors, semiconductors, graphite, conductive polymers and mixtures thereof
 12. The inductor of claim 11 wherein said first, second, third, and fourth windings comprise an electrically conductive material selected from the group consisting of transition metals, post-transition metals, carbon fiber and mixtures thereof
 13. The inductor of claim 12 wherein said first, second, third, and fourth windings comprise an electrically conductive material selected from the group consisting of copper, aluminum, gold, silver and mixtures thereof
 14. The inductor of claim 1, said inductor having a DC flux cancellation of from about 20% to about 95%.
 15. The inductor of claim 14, said inductor has a DC flux cancellation of from about 40% to about 95%.
 16. The inductor of claim 15, said inductor has a DC flux cancellation of from about 50% to about 90%.
 17. The inductor of claim 16, said inductor has a DC flux cancellation of from about 75% to about 90%.
 18. The inductor of claim 1, said inductor having a ratio of AC to DC current in said two other windings of from about 1:1 to about 1000000:1.
 19. The inductor of claim 18, said inductor has a ratio of AC to DC current in each of said AC said two other windings from about 2:1 to about 10000:1.
 20. The inductor of claim 19, said inductor has a ratio of AC to DC current in each of said two other windings from about 3:1 to about 1000:1.
 21. The inductor of claim 20, said inductor has a ratio of AC to DC current in each of said two other windings from about 4:1 to about 100:1.
 22. An article comprising an inductor according to claim 1, said article being selected from the group consisting of electrical current measurement or power converter and/or inverters.
 23. An article according to claim 22, said article being an electrical generation subsystem, electrical conditioning subsystem and/or distribution subsystem.
 24. An article according to claim 23, said article being a vehicle power conditioning subsystem, a hybrid and/or electric vehicle charging station, a motor drive, a renewable energy conditioning, laser and/or maser drive, a telecommunication transmission power conditioning system, or a wireless power transmission power conditioning system.
 25. A process of making an inductor comprising winding, around a core, a first winding, a second winding, a third winding and a fourth winding, said step of winding said first winding, said second winding, said third winding and said fourth winding about said core comprising winding said first winding, said second winding, said third winding and said fourth winding around said core pieces such that the following inductor conditions are met when L₁=L₃, L₂=L₄, M₁₂=M₃₄, and M₁₄=M₂₃: Equation For Said First Winding $V_{1} = {{L_{1}\frac{{di}_{1}}{dt}} + {M_{12}\frac{di_{2}}{dt}} - {M_{13}\frac{{di}_{3}}{dt}} - {M_{14}\frac{di_{4}}{dt}}}$ Equation For Said Second Winding $V_{1} = {{M_{12}\frac{di_{1}}{dt}} + {L_{2}\frac{di_{2}}{dt}} - {M_{23}\frac{{di}_{3}}{dt}} - {M_{24}\frac{di_{4}}{dt}}}$ Equation For Said Third Winding $V_{2} = {{{- M_{13}}\frac{di_{1}}{dt}} - {M_{23}\frac{{di}_{2}}{dt}} + {L_{3}\frac{di_{3}}{dt}} + {M_{34}\frac{{di}_{4}}{dt}}}$ Equation For Said Fourth Winding $V_{2} = {{{- M_{14}}\frac{{di}_{1}}{dt}} - {M_{24}\frac{{di}_{2}}{dt}} + {M_{34}\frac{{di}_{3}}{dt}} + {L_{4}\frac{di_{4}}{dt}}}$ wherein for said equations the variables are defined as follows: V₁ is a voltage across said first Winding; V₁ is a voltage across said second Winding; V₂ is a voltage across said third Winding; V₂ is a voltage across said fourth Winding; i₁ is a current in said first Winding; i₂ is a current in said second Winding; i₃ is a current in said third Winding; i₄ is a current in said fourth Winding; L₁ is a self inductance of said first Winding; L₂ is a self inductance of said second Winding; L₃ is a self inductance of said third Winding; L₄ is a self inductance of said fourth Winding; M₁₂ is a mutual inductance between said first Winding and said second Winding; M₁₃ is a mutual inductance between said first Winding and said third Winding; M₁₄ is a mutual inductance between said first Winding and said fourth Winding; M₂₃ is a mutual inductance between said second Winding and said third Winding; M₂₄ is a mutual inductance between said second Winding and said fourth Winding; M₃₄ is a mutual inductance between said third Winding and said fourth Winding; and said self and mutual inductances for said inductor satisfying one of the following set of conditions: Criteria 1 and Criteria 1a; Criteria 1 and Criteria 1b; Criteria 2 and Criteria 2a; or Criteria 2 and Criteria 2b; wherein said Criteria 1, Criteria 1a, Criteria 1b, Criteria 2, Criteria 2a, and Criteria 2b are as follows: L ₁ −M ₁₂≠0, M ₁₃ −M ₁₄≠0, and  (Criteria 1) $\frac{{di}_{1}}{dt} = {\frac{{di}_{3}}{dt} = 0}$ If V₁≠V₂, then $\frac{di_{2}}{dt}{and}\frac{di_{4}}{dt}$  are different values and: (M ₁₂ −L ₂)=(M ₁₄ −M ₂₄)=0  (Criteria 1a) If V₁=V₂, then $\frac{di_{2}}{dt} = \frac{di_{4}}{dt}$  and: (M ₁₂ −L ₂)=(M ₁₄ −M ₂₄)  (Criteria 1b) or M ₁₂ −L ₂≠0, M ₁₄ −M ₂₄≠0, and  (Criteria 2) $\frac{{di}_{2}}{dt} = {\frac{{di}_{4}}{dt} = 0}$ If V₁≠V₂, then $\frac{di_{1}}{dt}{and}\frac{di_{3}}{dt}$  are different values and: (L ₁ −M ₁₂)=(M ₁₃ −M ₁₄)=0  (Criteria 2a) If V₁=V₂, then $\frac{di_{2}}{dt} = \frac{di_{4}}{dt}$  and: (L ₁ −M ₁₂)=(M ₁₃ −M ₁₄)  (Criteria 2b).
 26. The process of claim 25 wherein said first winding, said second winding, said third winding and said fourth winding around said core such that said first winding and optionally said second winding pass through said winding passages of said core and after passing through said passages, said first winding is partially wound around said core and when said second winding passes through said winding passages of core, said second winding is partially wound around said core after passing through said passages of said core, said third winding and optionally said fourth winding passing through said winding passages of said core and after passing through said passages, said third winding is partially wound around said core, and when said fourth winding passes through said winding passages of said core, said fourth winding is partially wound around said core after passing through said passages of said core, said second winding is wound partially through said passages of said core, or being wound completely around said core and said fourth winding is wound partially through said passages of said core, or being wound completely around said core. 